Nuclear fission is the process of splitting atoms, or fissioning them. This
page will explain to you the basics of nuclear fission. Before we
talk about that, however, I would like to discuss marbles. Everyone's
played with marbles at one time or another, right? Well, imagine about 200
marbles lying on a flat surface, all jumbled together, and roughly forming
a circle. What would happen
if someone took another marble and threw it at them? They would fly all
around in different directions and groups, right? That is exactly what
happens in nuclear fission. The filled circle is like an atom's nucleus. The marble being thrown is like a "neutron bullet". The only differences are that
the marbles are protons and neutrons and the protons and neutrons aren't in a
filled circle, but in the actual atom are in the shape of a sphere. Of course,
an atom is also a bit more complicated than a pack of marbles.
Choosing the Bullet:
When we spoke about the marble analogy earlier, we said that the marble being
thrown is a like a "neutron bullet". But what does this mean, and why not use
another type of particle to "throw" at a nucleus to fission it? First, what
particles with distinct mass are available to launch at a nucleus? Think back
to our lesson on radioactivity. Recall that two particles emitted by
radioactive elements are the particle and the neutron. (There are other
particles emitted too, but they are generally much smaller than the neutron and
the particle.) Recall that the
particle is essentially a 4He nucleus. Now, let's
review the structure of an atom. Remember that an atomic nucleus is
made up of positive protons and neutral neutrons? Because of this, the nucleus
carries an overall positive charge. So, if we were to launch another particle
with a positive charge at a nucleus, it wouldn't get there. Why wouldn't it get
there? The answer lies in magnetism. Have you ever used
magnets? If you have, you'd know that two like poles of a magnet repel each
other. A positive particle and the positive nucleus would repel each other in
the same way. The particle is positive. Why? Well, it's composed of
two protons and two neutrons. Its positive protons give it a positive charge.
Because it's positive, it would get repelled away from another positive nucleus.
So, the only thing left is the neutron. The neutron is electrically neutral
and thus would not get repelled from a positive nucleus.
Fissile Isotopes:
Fissile isotopes are isotopes of an element that can be split through fission.
Only certain isotopes of certain elements are fissile. For example, one isotope
of uranium, 235U, is fissile, while another isotope,
238U, is not. Other examples of fissile elements are
239Pu and 232Th. An important
factor affecting whether or not an atom will fission is the speed at which
the bombarding neutron is moving. If the neutron is highly energetic (and thus
moving very quickly), it can cause fission in some elements that a slower
neutron would not. For example, thorium 232 requires a very fast neutron to
induce fission. However, uranium 235 needs slower neutrons. If a neutron is
too fast, it will pass right through a 235U atom without
affecting it at all.
Splitting the Uranium Atom:
Uranium is the principle element used in nuclear reactors and in certain types
of atomic bombs. The specific isotope used is 235U.
When a stray neutron strikes a
235U nucleus, it is at first absorbed into it. This creates
236U. 236U is unstable and this causes the atom to
fission. The fissioning of 236U can produce over twenty different
products. However, the products' masses always add up to 236. The following
two equations are examples of the different products that can be produced when
235U fissions:
Let's discuss those reactions. In each of the above reactions, 1 neutron splits
the atom. When the atom is split, 1 additional neutron is released. This is
how a chain reaction works. If more 235U is present,
those 2 neutrons can cause 2 more atoms to split. Each of those atoms releases
1 more neutron bringing the total neutrons to 4. Those 4 neutrons can strike 4
more 235U atoms, releasing even more neutrons. The
chain reaction will continue until all the 235U fuel is
spent. This is
roughly what happens in an atomic bomb. It is called a runaway nuclear
reaction.
In this animation, one can see how the fissioning of each 235U
atom (red) releases more neutrons (green) that go on to fission more
235U atoms, thus producing a chain reaction.
Where Does the Energy Come From?:
In the section above we described what happens when an 235U
atom fissions. We gave the following equation as an example:
You might have been wondering, "Where does the energy come from?". The mass
seems to be the same on both sides of the reaction:
235 + 1 = 2 + 92 + 142 = 236
Thus, it seems that no mass is converted into energy. However, this is not
entirely correct. The mass of an atom is more than the sum of the individual
masses of its protons and neutrons, which is what those numbers represent.
Extra mass is a result of the binding energy that holds the
protons and neutrons of the nucleus together.
Thus, when the uranium atom is split, some of the energy that held it
together is released as radiation in the form of heat. Because energy and mass
are one and the same, the energy released is also mass released. Therefore,
the total mass does decrease a tiny bit during the reaction.
Quiz time (feel free to re-look at the above material while completing the quiz):
Runaway Reactions:
Earlier, we explained the concept of a chain reaction, in which neutrons are
released and then produce more reactions that release more neutrons.
The first neutron is a first generation neutron. This can release between
2-3 more neutrons, depending on the way in which the uranium nucleus splits.
We will assume that about 2.5 neutrons are released during each fissioning.
Those 2.5 neutrons are second generation neutrons. Then, those 2.5 second
generation neutrons prompt the fissioning of more uranium, producing
approximately
2.5 third generation neutrons, for each second generation neutron. So, the
total number of neutrons in the third generation is now: 2.5 x 2.5, or
6.25
neutrons.
In a nuclear reactor, there is approximately 1 millisecond between each
generation. So, what does this mean? It means that every millisecond, the
number of neutrons increases 2.5 times. So, if at time 0, there are 5 neutrons
present, 10 milliseconds later, there are 5x 2.510
=47,683.7158, or about 47,700 neutrons. That's a lot of free
neutrons to be created in .01 seconds!
So, for our first question:
If each time the 235U nucleus fissions, 2.5 neutrons are released,
and there is one millisecond between each generation, how many neutrons are free
after an eighth of a second (125 milliseconds) of a runaway reaction that is
initiated by one free neutron? Warning!! This will be an extremely large
number.
If we assume that each time 235U is split it produces 2.5 more
neutrons, and there is one millisecond between each reaction, how many
milliseconds would it take for there to be at least 500,000 free neutrons?
In a nuclear reactor we don't want a runaway nuclear reaction. That would
essentially be a nuclear bomb!! (I don't know about you, but I don't want
a
nuclear bomb going off in the power station in my back yard.) However, we do
want the nuclear reactions
to continue and still give off energy. This requires moderation. Unchecked,
as we said earlier, each nuclear reaction generation will produce 2.5 times
as many neutrons as went into it. However, in order to maintain stability
(and to keep the chain reaction from running away from itself), each generation of
reactions in a nuclear power plant must produce exactly the same number of
neutrons as went into it. So, if a normal nuclear fission of one
atom of 235U produces 2.5 neutrons, approximately how many
neutrons per atom need
to be kept from moving on to the next generation?